Kinetic Theory of Gases
The kinetic theory of gases connects the microscopic motion of molecules with the macroscopic properties of gases. Let’s derive its key results step by step.
1. Molecule in a Cube
Imagine a cube of side L containing a single gas molecule of mass m. Its velocity has components \(v_x, v_y, v_z\).
2. Momentum Change
On colliding with a wall perpendicular to the x-axis, momentum reverses: from \(+mv_x\) to \(-mv_x\). Hence, change = \(-2mv_x\). This momentum is transferred to the wall.
3. Time Between Collisions
The molecule must travel to the opposite wall and back before colliding again. Distance = \(2L\), speed = \(v_x\), so time = \(2L / v_x\).
4. Average Force
Force = (change in momentum) ÷ (time interval). Substituting: \(F = (2mv_x) / (2L/v_x) = m v_x^2 / L\).
5. Pressure from One Molecule
Pressure = Force ÷ Area. Area of wall = \(L^2\). Thus, \(P = (m v_x^2 / L) ÷ L^2 = m v_x^2 / V\).
6. Total Pressure from N Molecules
For N molecules, we sum their contributions. Using average square velocity: \(⟨v_x^2⟩\).
7. Velocity Components
Since motion is random and isotropic, energy is equally distributed among x, y, z directions. So the mean square speed along one axis is one-third of the total.
8. Final Pressure Formula
Let \(\rho = Nm/V\) (density), and define root mean square speed \(v_{rms} = \sqrt{⟨v²⟩}\). Then: \(P = \tfrac{1}{3}\rho v_{rms}^2\).
9. RMS Speed Expression
Relating kinetic energy to temperature: \(\tfrac{1}{2}m⟨v^2⟩ = \tfrac{3}{2}kT\). In molar form, \(v_{rms} = \sqrt{3RT/M}\).
10. Examples
Interactive Demo: Effect of Temperature
Adjust the temperature to see how RMS speed changes.
RMS Speed of O₂: 0 m/s
Key Takeaways
- Gas pressure arises from collisions of molecules with container walls.
- Temperature is a direct measure of average kinetic energy.
- The Kinetic Theory explains macroscopic gas laws using microscopic motion.
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